Method and apparatus providing refractive index structure for a device capturing or displaying images

ABSTRACT

A transient index stack having an intermediate transient index layer, for use in an imaging device or a display device, that reduces reflection between layers having different refractive indexes by making a gradual transition from one refractive index to another. Other embodiments include a pixel array in an imaging or display device, an imager system having improved optical characteristics for reception of light by photosensors and a display system having improved optical characteristics for transmission of light by photoemitters. Enhanced reception of light is achieved by reducing reflection between a photolayer, for example, a photosensor or photoemitter, and surrounding media by introducing an intermediate layer with a transient refractive index between the photolayer and surrounding media such that more photons reach the photolayer. The surrounding media can include a protective layer of optically transparent media.

FIELD OF THE INVENTION

The invention relates to solid state imagers, display devices, and moreparticularly to optical paths used in solid state imagers and displaydevices.

BACKGROUND OF THE INVENTION

Solid state imagers generate electrical signals in response to lightreflected by an object being imaged. Complementary metal oxidesemiconductor (CMOS) imagers are one of several different known types ofsemiconductor-based imagers, which include for example, charge coupleddevices (CCDs), photodiode arrays, charge injection devices and hybridfocal plane arrays.

Some inherent limitations in CCD technology have promoted an increasinginterest in CMOS imagers for possible use as low cost imaging devices. Afully compatible CMOS imager technology enabling a higher level ofintegration of an image array with associated processing circuits wouldbe beneficial to many digital image capture applications. CMOS imagershave a number of desirable features, including for example low voltageoperation and low power consumption. CMOS imagers are also compatiblewith integrated on-chip electronics (control logic and timing, imageprocessing, and signal conditioning such as A/D conversion). CMOSimagers allow random access to the image data, and have lowermanufacturing costs, as compared with conventional CCDs, since standardCMOS processing techniques can be used to fabricate CMOS imagers.Additionally, CMOS imagers have low power consumption because only onerow of pixels needs to be active at any time during readout and there isno charge transfer (and associated switching) from pixel to pixel duringimage acquisition. On-chip integration of electronics is particularlydesirable because of the potential to perform many signal conditioningfunctions in the digital domain (versus analog signal processing) aswell as to achieve reductions in system size and cost.

Nevertheless, demands for enhanced resolution of CCD, CMOS and othersolid state imaging devices, and a higher level of integration ofimaging arrays with associated processing circuitry, are accompanied bya need to improve the light sensing characteristics of the pixels of theimaging arrays. For example, it would be beneficial to minimize, if noteliminate, the loss of light transmitted to individual pixels duringimage acquisition and the amount of crosstalk between pixels caused bylight being scattered or shifted from one pixel to a neighboring pixel.

A significant source of photon reflection can occur at the junction ofdifferent media, each having a different refractive index. Photonreflection between two different media can be expressed by the followingformula:$R = \frac{\left( {n_{1} - n_{2}} \right)^{2}}{\left( {n_{1} + n_{2}} \right)^{2}}$where n₁ and n₂ are the refractive indices of the two media and R is thepercentage of photons reflected at the junction of the two media.

Silicon and silicon oxide layers are required in many conventional CMOSphotosensor structures because of the limitations of conventional CMOStechnology and the high quantum efficiency of a crystallized siliconbased photodiode.

With reference to FIGS. 1(a)-(c), which respectively illustrate atop-down view, a partial cross-sectional view and electrical circuitschematic of a conventional CMOS pixel sensor cell 100, when incidentlight 187 strikes the surface of a photosensor (photodiode) 120,electron/hole pairs are generated in the p-n junction of the photosensor(represented at the boundary of n-type accumulation region 122 andp-type surface layer 123 [FIG. 1(b)]). The generated electrons(photo-charges) are collected in the n-type accumulation region 122 ofthe photosensor 120. The photo-charges move from the initial chargeaccumulation region 122 to a floating diffusion region 110 via atransfer transistor 106. The charge at the floating diffusion region 110is typically converted to a pixel output voltage by a source followertransistor 108 and then output on a column output line 111 via a rowselect transistor 109.

Conventional CMOS imager designs, such as that shown in FIGS. 1(a)-(c)for pixel cell 100, include a substrate 101 having a photosensor 120 andisolation regions 102. The floating diffusion region 110 is coupled to atransfer transistor gate 106′ of the transfer transistor 106.Source/drain regions 115 are provided for reset 107, source follower108, and row select 109 transistors which have respective gates 107′,108′, and 109′. A silicon dioxide layer 150 is typically formed over thesubstrate 101 to form a silicon-silicon dioxide stack, for example, as aprotective layer.

A silicon/silicon dioxide stack 20 is shown in FIG. 2(a). A first layer22 having a first refractive index, which corresponds to silicon dioxidelayer 150 of FIG. 1(b), is formed on a second layer 21 having a secondrefractive index, corresponding to silicon substrate 101 of FIG. 1(b).However, formation of silicon dioxide on top of a silicon photodiode canlead to significant reflection at the junction of the two layers. Wherethe first layer is silicon dioxide (at or about n=1.45) and the secondlayer is silicon (at or about n=4), the stack 20 produces reflection Rof about 22% of photons at the junction 23 of the first and secondlayers.

FIG. 2(b) shows a plot of the refractive index n of the stack of FIG.2(a) relative to depth d. At the depth of junction 23, the refractiveindex n rises sharply from 1.5 to 4.0. FIG. 2(c) shows a plot of thetotal reflection R within the stack of FIG. 2(a) relative to depth d. Atthe junction 23, where n jumps from 1.5 to 4.0, the percentagereflection R spikes to 22%, which is undesirable. Referring back to FIG.1(b), a significant quantity of photons is reflected at the junctionbetween substrate 101 and silicon dioxide layer 150, and thus are notdetected by the imager.

Accordingly, there is a need and desire for an improved solid stateimaging device, capable of receiving and propagating light with minimalloss of light transmission to a photosensor. There is also a need anddesire for improved fabrication methods for imaging devices that providea high level of light transmission to the photosensor and reduce thelight scattering drawbacks of the prior art, such as crosstalk andphoton reflection.

There is also a need for improved display devices which utilize an arrayof photoemitters for light emission which also have improved lightpropagating properties.

BRIEF SUMMARY OF THE INVENTION

Exemplary embodiments of the invention provide a transient index stackhaving an intermediate transient index layer, for use in an imagingdevice or a display device, that reduces reflection between layershaving different refractive indexes by making a gradual transition fromone refractive index to another. Other embodiments include a pixel arrayin an imaging or display device, an imager system having improvedoptical characteristics for reception of light by photosensors and adisplay system having improved optical characteristics for transmissionof light by photoemitters. Enhanced reception of light is achieved byreducing reflection between a photolayer, for example, a photosensor orphotoemitter, and surrounding media by introducing an intermediate layerwith a transient refractive index between the photolayer and surroundingmedia such that more photons reach the photolayer. The surrounding mediacan include a protective layer of optically transparent media.

Methods for forming an imaging device, in accordance with exemplaryembodiments of the invention, include forming one or more intermediatetransient index layers between media layers, having different indexes ofrefraction, disposed over focal plane arrays of photosensors. Theexemplary methods include the acts of forming photosensors on a wafer,providing an intermediate transient index layer, and providing anoptically transparent medium over the intermediate transient indexlayer, for example, as a protective layer. A color filter layer may alsobe fabricated with an individual color filter over a respectivephotosensor/intermediate transient index layer stack and a microlensstructure layer can be fabricated over the color filter layer.

Also disclosed are structures and fabrication methods for optical pathsused in display devices which have improved optical characteristics fortransmission of light from photoemitters.

These and other features and advantages of the invention will be moreapparent from the following detailed description that is provided inconnection with the accompanying drawings illustrating exemplaryembodiments of the invention.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1(a) is a top-down view of a conventional four transistor CMOSpixel cell.

FIG. 1(b) is a cross-sectional view of the pixel cell of FIG. 1(a),taken along line 1-1′.

FIG. 1(c) is a circuit diagram of the conventional CMOS pixel of FIGS.1(a) and (b).

FIG. 2(a) is a cross sectional view of an optical stack having a silicondioxide layer formed on a silicon layer according to the prior art.

FIG. 2(b) is a plot of the transient index n of the stack of FIG. 2(a)relative to depth d.

FIG. 2(c) is a plot of the total reflection R within the stack of FIG.2(a) relative to depth d.

FIG. 3(a) is a cross sectional view of a stack having a silicon dioxidelayer formed on a silicon layer and also having an intermediatetransient index stack in accordance with a first exemplary embodiment ofthe invention.

FIG. 3(b) is a plot of the transient index n of the stack of FIG. 3(a)relative to depth.

FIG. 3(c) is a plot of the percentage reflection R within the stack ofFIG. 3(a) relative to depth d.

FIG. 4(a) is a cross sectional view of a stack having a silicon dioxidelayer formed on a silicon layer and also having an intermediatetransient index stack in accordance with a second exemplary embodimentof the invention.

FIG. 4(b) is a plot of the transient index n of a stack of FIG. 4(a),relative to depth.

FIG. 4(c) is a plot of the percentage reflection R within the stack ofFIG. 4(a) relative to depth d.

FIG. 4(d) is a plot of the total percentage reflection of all lightpassing through the stack according to the second exemplary embodimentin relation to the number of discrete transient index layers.

FIG. 5(a) is a cross sectional view of a stack having a silicon dioxidelayer formed on a silicon layer and also having an intermediatetransient index stack in accordance with a third exemplary embodiment ofthe invention.

FIG. 5(b) is a plot of the transient index n of a stack of FIG. 5(a),relative to depth.

FIG. 5(c) is a plot of the percentage reflection R within the stack ofFIG. 5(a) relative to depth d.

FIG. 6 is a cross-sectional view of a CMOS pixel cell comprising anintermediate transient layer according to the invention.

FIG. 7 depicts a block diagram of an imager device constructed inaccordance with an embodiment of the invention.

FIG. 8 depicts a processor system incorporating at least one imagerdevice constructed in accordance with an embodiment of the invention.

DETAILED DESCRIPTION

In the following detailed description, reference is made to variousspecific embodiments which exemplify the invention. These embodimentsare described with sufficient detail to enable those skilled in the artto practice the invention, and it is to be understood that otherembodiments may be employed, and that structural and logical changes maybe made without departing from the spirit or scope of the invention.

The term “substrate” used in the following description may include anysemiconductor-based structure. The structure should be understood toinclude silicon, silicon-on insulator (SOI), silicon-on-sapphire (SOS),doped and undoped semiconductors, epitaxial layers of silicon supportedby a base semiconductor foundation, and other semiconductor structures.The semiconductor need not be silicon-based. The semiconductor could besilicon-germanium, germanium, or gallium arsenide. When reference ismade to the substrate in the following description, previous processsteps may have been utilized to form regions or junctions in or over thebase semiconductor or foundation.

An intermediate layer having a transient refractive index isparticularly advantageous when formed between a silicon photosensorlayer and a protective silicon dioxide layer such as those found in,e.g., CMOS imager pixel cells. The intermediate layer may be formed bydifferent methods, for example, by silicon quantum dot formation, byreactive physical vapor deposition (“PVD”), or by chemical vapordeposition (“CVD”).

Silicon quantum dot formation creates silicon “dots” each having adiameter smaller than the wavelength of visible light in an intermediatesilicon dioxide layer. By forming dots such that the size and/ordistribution density of the dots decreases uniformly from the siliconlayer to the silicon dioxide layer, the reflection is minimized at thejunctions of the intermediate layer and the respective silicon andsilicon dioxide layers, and throughout the intermediate layer.

Reactive PVD and CVD deposition can also generate an intermediate layerhaving reduced photon reflection by gradually increasing oxygen flowduring deposition of silicon. By controlling the oxygen flow as afunction of deposition time, the resultant intermediate transient layerhas a smooth transition from pure silicon to silicon dioxide.

FIG. 3(a) is a cross sectional view of an optical stack 30 formed inaccordance with a first exemplary embodiment of the invention. The stack30 comprises a silicon base layer 31, a silicon dioxide layer 32 and anintermediate transient layer 33 between layers 31 and 32. Theintermediate transient layer 33 has a refractive index at or about n=4.0at the junction 34 between the silicon base layer 31 and theintermediate transient layer 33 and a refractive index at or about n=1.5at the junction 35 between the silicon dioxide layer 32 and theintermediate transient layer 33. The refractive index n of theintermediate transient layer gradually transitions from at or aboutn=1.5 at junction 34 to at or about n=4.0 at junction 35, therebyreducing reflection at the junctions 34, 35 and throughout theintermediate transient layer 33.

The intermediate transient layer may be formed on a silicon substrate,for example, by adding silicon dioxide in increasing proportion duringlayer formation until a pure silicon dioxide layer is achieved. Morespecifically, an intermediate transient index may be formed on a siliconsubstrate by using reactive sputter PVD deposition of silicon; bygradually increasing flow of oxygen during the reactive sputterdeposition, the refractive index n of the intermediate transient indexlayer would gradually increase from at or about n=1.5 to at or aboutn=4.0 for example. Similarly, CVD deposition can achieve the sameresults, by increasing the proportion of precursors as a function oflayer depth.

FIG. 3(b) is a plot of the transient refractive index n of the stack ofFIG. 3(a) relative to depth d. Unlike the plot shown in FIG. 2(b), FIG.3(b) shows a change in refractive index n relative to depth d that ismore gradual and less abrupt than at the junction 23 in FIG. 2(b).

FIG. 3(c) shows a plot of the total reflection R within the stack ofFIG. 3(a) relative to depth d. Here, the reflection increases with thechange in n shown in FIG. 3(b), but to a lesser extent than in theconventional stack 20, as shown in FIGS. 2(a) and 2(c). Fewer photonsare reflected at junction, and many photons can be recovered once theyenter the intermediate transient layer because the same change inrefractive index n will re-reflect a percentage of the reflected photonsback in the correct direction. This photon recovery is not possible withthe conventional stack 20 of FIG. 2(a), which has no way to re-reflectphotons that have been reflected at junction 23.

FIG. 4(a) is a cross sectional view of a stack 40 having a silicondioxide layer 42 formed over a silicon layer 41 and with an intermediatetransient index stack 43 in accordance with a second exemplaryembodiment of the invention formed therebetween. In this embodiment,discrete layers 43(a)-(f) having incrementally larger refractive indexesin the direction of the substrate are formed over the silicon substrate41. In the illustrated embodiment, beginning with a silicon substrate41, each discrete intermediate layer 43(a)-(f) has an incrementallyhigher proportion of silicon dioxide than the prior layer, ultimatelyreaching pure silicon dioxide concentration in the final layer 43(a). Auniform silicon dioxide layer 42 may then be formed over theintermediate transient index stack 43.

FIG. 4(b) is a plot of the transient refractive index n of the stack ofFIG. 4(a) relative to depth d. Here, the change in refractive index nrelative to depth d takes place incrementally and reduces overallreflection. FIG. 4(c) is a plot of the percentage reflection R withinthe stack of FIG. 4(a) relative to depth d. The percentage reflection Ris dispersed into a series of smaller spikes at the junction betweeneach layer 43(a)-(f) than the single large spike of FIG. 2(c). Thespikes at each junction may also re-reflect and thereby recoverreflected photons.

The embodiment shown in FIG. 4(a) uses 6 discrete layers 43(a)-(f), butany number of layers may be used with varying results, as discussedbelow with respect to FIG. 4(d).

One advantage of the embodiment illustrated in FIG. 4(a) over theembodiment illustrated in FIG. 3(a) is reduced cost of fabrication. Insituations where a tradeoff between fabrication cost and percentage ofphoton reflection is permitted, fabrication cost can be dramaticallyreduced by employing fewer discrete layers during fabrication. FIG. 4(d)is a plot of the total reflection percentage of an optical stackaccording to the second exemplary embodiment in relation to the numberof discrete transient index layers, illustrating the cost/benefittradeoff between the number of discrete layers and overall reflection.With a greater number of discrete layers, the change in refractive indexn at each junction is less drastic, and produces a smaller series ofspikes in reflection percentage R.

FIG. 5(a) is a cross sectional view of a stack 50 having a silicondioxide layer 52 formed on a silicon layer 51 and also having anintermediate transient index stack in accordance with a third exemplaryembodiment of the invention. FIG. 5(a) shows an intermediate silicondioxide transient layer containing silicon quantum dots 53 formedtherein. By using quantum dots 53 smaller than the wavelength of visiblelight (<0.2 um) and by adjusting the distribution density of the dots 53in the intermediate transient index layer, the layer can be madeoptically equivalent to the optimum intermediate transient index layer33 of FIG. 3(a).

FIG. 5(b) is a plot of the transient refractive index n of the stack ofFIG. 5(a) relative to depth d. Like FIG. 3(b), FIG. 5(a) shows a changein refractive index n relative to depth d that is smoother and lessabrupt than at the junction 23 in FIG. 2(b). FIG. 5(c) is a plot ofpercentage reflection relative to depth d which, like FIG. 3(c),produces less total reflection than the optical stack of FIG. 2(a).

The methods of forming the intermediate transient index layer areflexible and can be adjusted according to the tolerances and desiredoptical characteristics of the imaging or display device.

FIG. 6 illustrates the use of an optical stack, e.g., stacks 30, 40, 50,according to the invention in an imager pixel cell 100′, with layer 151corresponding to an intermediate transient layer according to any one ofthe embodiments described above. The remainder of the cell 100′ may bethe same as the conventional cell 100 (FIG. 1(b)).

FIG. 7 illustrates a block diagram of an exemplary CMOS imager 108having a pixel array 140 comprising a plurality of pixel cells 100′arranged in a predetermined number of columns and rows, with each pixelcell being constructed as illustrated and described above with respectto FIG. 6. Other known pixel architectures may be used, but all willinclude intermediate transient layer 151 as described above with respectto FIG. 6. Attached to the pixel array 140 is signal processingcircuitry for controlling the pixel array 140, as described herein, atleast part of which may be formed in the substrate. The pixel cells ofeach row in array 140 are all turned on at the same time by a row selectline, and the pixel cells of each column are selectively output byrespective column select lines. A plurality of row select and columnselect lines are provided for the entire array 140. The row lines areselectively activated by a row driver 145 in response to row addressdecoder 155. The column select lines are selectively activated by acolumn driver 160 in response to column address decoder 170. Thus, a rowand column address is provided for each pixel cell.

The CMOS imager 108 is operated by a timing and control circuit 152,which controls address decoders 155, 170 for selecting the appropriaterow and column lines for pixel readout. The control circuit 152 alsocontrols the row and column driver circuitry 145, 160 such that theyapply driving voltages to the drive transistors of the selected row andcolumn lines. The pixel column signals, which typically include a pixelreset signal V_(rst) and a pixel image signal V_(sig), are output tocolumn driver 160, on output lines, and are read by a sample and holdcircuit 161. V_(rst) is read from a pixel cell 100′ immediately afterthe floating diffusion region 110 is reset. V_(sig) represents theamount of charges generated by the photosensitive element of the pixelcell 100′ in response to applied light during an integration period. Adifferential signal (V_(rst)−V_(sig)) is produced by differentialamplifier 162 for each readout pixel cell. The differential signal isdigitized by an analog-to-digital converter 175 (ADC). The analog todigital converter 175 supplies the digitized pixel signals to an imageprocessor 180, which forms and outputs a digital image.

FIG. 8 illustrates a processor-based system 1100 includes an imagingdevice 108 constructed in accordance with an embodiment of theinvention, CPU 1102, RAM 1110, I/O device 1106, and removable memory1115. As discussed above, the imaging device 108 contains a pixel array140 having a plurality of pixel cells 100′, each having a transientindex stack formed and used as described herein. The processor-basedsystem 1100 is exemplary of a system having digital circuits that couldinclude image sensor devices. Without being limiting, such a systemcould include a computer system, camera system, scanner, machine vision,vehicle navigation, video phone, surveillance system, auto focus system,star tracker system, motion detection system, image stabilizationsystem, and other image sensing and/or processing system.

The processor-based system 1100, for example a camera system, generallycomprises a central processing unit (CPU) 1102, such as amicroprocessor, that communicates with an input/output (I/O) device 1106over a bus 1104. Imaging device 308 also communicates with the CPU 1102over the bus 1104. The processor-based system 1100 also includes randomaccess memory (RAM) 1110, and can include removable memory 1115, such asflash memory, which also communicates with CPU 1102 over the bus 1104.Imaging device 308 may be combined with a processor, such as a CPU,digital signal processor, or microprocessor, with or without memorystorage on a single integrated circuit or on a different chip than theprocessor. The above techniques, structure and system can be applied todisplay devices employing photoemitters as well. For example, a pixelarray similar to the array 140 of FIG. 7, but employing photoemittersemploying the present invention rather than photosensors, may be used ina display device to reduce internal reflection and to emit a moreaccurate signal.

The above description and drawings are only to be consideredillustrative of exemplary embodiments which achieve the features andadvantages of the invention. Modification of, and substitutions to,specific process conditions and structures can be made without departingfrom the spirit and scope of the invention. Accordingly, the inventionis not to be considered as being limited by the foregoing descriptionand drawings, but is only limited by the scope of the appended claims.

1. An optical structure for an imaging device comprising: a photodevice, and an associated optical path for the photo device, saidoptical path comprising: a first layer comprising a first materialhaving a first refractive index; a second layer comprising a secondmaterial having a second refractive index; and a transition regionbetween said first and second layers having a refractive index whichchanges from a value at or about said first refractive index to a valueat or about said second refractive index.
 2. The optical structureaccording to claim 1, wherein said transition region comprises a mixtureof said first and second materials; and wherein a ratio of said firstmaterial to said second material in said mixture increases in thedirection of the optical path toward the second layer.
 3. The opticalstructure according to claim 2, wherein said first material is silicondioxide and said second material is silicon.
 4. The optical structureaccording to claim 3, wherein said silicon is provided as a substratefor said photo device.
 5. The optical structure according to claim 2,wherein the increase in the ratio of said first material to said secondmaterial in said mixture in the direction of the optical path isproportional to depth in the direction of the optical path toward thesecond layer.
 6. The optical structure according to claim 2, wherein thetransition region comprises quantum dots of said second material withina layer of said first material.
 7. The optical structure according toclaim 2, wherein the transition region comprises a stack of discretetransition layers, each layer comprising a uniform mixture of said firstand second materials.
 8. The optical structure according to claim 7,wherein the ratio of said first material to said second material in eachdiscrete transition layer increases incrementally in the direction ofthe second layer.
 9. The optical structure according to claim 1, whereinthe imaging device is adapted to capture an image and said photo deviceis a photosensor.
 10. The optical structure according to claim 1,wherein the imaging device is adapted to display an image and said photodevice is a photoemitter.
 11. A method of forming an optical structurefor an imaging device comprising: providing a photo device, and formingan associated optical path for the photo device, said optical path beingformed by: providing a first layer comprising a first material having afirst refractive index; providing a layer comprising a second materialhaving a second refractive index; and providing a transition regionbetween said first and second layers having a refractive index whichchanges from a value at or about said first refractive index to a valueat or about said second refractive index.
 12. The method according toclaim 11, wherein said transition region comprises a mixture of saidfirst and second materials; and wherein a ratio of said first materialto said second material in said mixture increases in the direction ofthe optical path toward the second boundary
 13. The method according toclaim 12, wherein said first material is silicon dioxide and said secondmaterial is silicon.
 14. The method according to claim 13, wherein saidsilicon is provided as a substrate for said photo device.
 15. The methodaccording to claim 12, wherein the increase in the ratio of said firstmaterial to said second material in said mixture in the direction of theoptical path is proportional to depth in the direction of the opticalpath toward the second layer.
 16. The method according to claim 12,wherein the transition region comprises quantum dots of said secondmaterial within a layer of said first material.
 17. The method accordingto claim 12, wherein the transition region comprises a stack of discretetransition layers, each layer comprising a uniform mixture of said firstand second materials.
 18. The method according to claim 17, wherein theratio of said first material to said second material in each discretetransition layer increases incrementally in the direction of the secondlayer.
 19. The method according to claim 11, wherein the imaging deviceis adapted to capture an image and said photo device is a photosensor.20. The method according to claim 11, wherein the imaging device isadapted to display an image and said photo device is a photoemitter. 21.The method according to claim 11, wherein the transition region isformed by chemical vapor deposition.
 22. The method according to claim11, wherein the transition region is formed by physical vapordeposition.
 23. An imaging system comprising: a CPU; and an imagingdevice comprising and optical structure, said optical structurecomprising: a photo device, and an associated optical path for the photodevice, said optical path comprising: a first layer comprising a firstmaterial having a first refractive index; a second layer comprising asecond material having a second refractive index; and a transitionregion between said first and second layers having a refractive indexwhich changes from a value at or about said first refractive index to avalue at or about said second refractive index.
 24. The system accordingto claim 23, wherein said transition region comprises a mixture of saidfirst and second materials; and wherein a ratio of said first materialto said second material in said mixture increases in the direction ofthe optical path toward the second layer.
 25. The system according toclaim 24, wherein said first material is silicon dioxide and said secondmaterial is silicon.
 26. The system according to claim 25, wherein saidsilicon is provided as a substrate for said photo device.
 27. The systemaccording to claim 24, wherein the increase in the ratio of said firstmaterial to said second material in said mixture in the direction of theoptical path is proportional to depth in the direction of the opticalpath toward the second layer.
 28. The system according to claim 24,wherein the transition region comprises quantum dots of said secondmaterial within a layer of said first material.
 29. The system accordingto claim 24, wherein the transition region comprises a stack of discretetransition layers, each layer comprising a uniform mixture of said firstand second materials.
 30. The system according to claim 29, wherein theratio of said first material to said second material in each discretetransition layer increases incrementally in the direction of the secondlayer.
 31. The system according to claim 23, wherein the imaging deviceis adapted to capture an image and said photo device is a photosensor.32. The system according to claim 23, wherein the imaging device isadapted to display an image and said photo device is a photoemitter.